We study the effects of short-range interactions on a generalized three-dimensional Weyl semimetal, where the band touching points act as the (anti)monopoles of Abelian Berry curvature of strength n. We show that any local interaction has a negative scaling dimension −2/n. Consequently all Weyl semimetals are stable against weak short-range interactions. For sufficiently strong interactions, we demonstrate that the Weyl semimetal either undergoes a first order transition into a band insulator or a continuous transition into a symmetry breaking phase. A translational symmetry breaking axion insulator and a rotational symmetry breaking semimetal are two prominent candidates for the broken symmetry phase. At one loop level, the correlation length exponent for continuous transitions is ν = n/2, indicating their non-Gaussian nature for any n > 1. We also discuss scaling of thermodynamic and transport quantities inside the broken symmetry phases.Introduction: There is tremendous ongoing interest in three dimensional, gapless topological systems [1][2][3][4][5][6]. An interesting class of such systems is described by the isolated nodal points of time reversal or inversion symmetry breaking materials, where two non-degenerate bands touch [7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25]. These points are known as Weyl points, which act as the (anti)monopoles or (anti)hedgehog of Abelian Berry curvature. For a general monopole strength n (with only n = 1, 2, 3 in crystalline systems), the dispersion relations around the nodal points acquire the form ± (k) ∼ ± v 2 k 2 z + α 2 n k 2n ⊥ , which can be observed in ARPES experiments [22,23], where k